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Topic 3 Dielectric Waveguides and Optical Fibers 2-1 Symmetric ...

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Example 2.3.4: Group velocity <strong>and</strong> delay<br />

Consider a single mode fiber with core <strong>and</strong> cladding indices of 1.448<br />

<strong>and</strong> 1.440, core radius of 3μm, operating at 1.5μm. Given that<br />

we can approximate the fundamental mode normalized<br />

propagation constant b by<br />

901 37500 光電導論<br />

b ≈ (1.1428 – 0.996 / V ) 2 1.5 < V < 2.5<br />

(1) Calculate the propagation constant β.<br />

(2) Change the operating wavelength to λ’ by a small amount,<br />

0.01%, <strong>and</strong> then recalculate the new propagation constant β’.<br />

(3) Then determine the group velocity v g of the fundamental mode at<br />

1.5μm, <strong>and</strong> the group delay τ g over 1 km of fiber.<br />

αα max<br />

n 0<br />

901 37500 光電導論<br />

n 2<br />

n 1<br />

θ < θ c<br />

Fiber axis<br />

Lost<br />

B<br />

θ > θ c<br />

Cladding<br />

Core<br />

©1999 S.O. Kasap, Optoelectronics (Prentice Hall)<br />

Propagates<br />

A<br />

37<br />

Maximumacceptance angle<br />

α max is that which just gives<br />

totalinternalreflectionatthe<br />

core-cladding interface, i.e.<br />

when α=α maxthen θ=θ c.<br />

Rays with α>α max (e.g. ray<br />

B) become refracted <strong>and</strong><br />

penetrate the cladding <strong>and</strong> are<br />

eventually lost.<br />

39<br />

901 37500 光電導論<br />

Snell’s law --><br />

Numerical Aperture<br />

901 37500 光電導論<br />

2-4 Numerical Aperture<br />

Maximum acceptance<br />

angle α max<br />

sinα<br />

max n<br />

=<br />

<br />

sin( 90 −θ ) n<br />

sinα<br />

max<br />

=<br />

c<br />

1<br />

0<br />

2 2 ( n − n )<br />

1<br />

n<br />

0<br />

( ) 2 / 1 2 2<br />

n n<br />

NA = −<br />

sinα<br />

max<br />

1<br />

=<br />

0<br />

2<br />

NA<br />

n<br />

2πa<br />

V = NA<br />

λ<br />

1/<br />

2<br />

2<br />

38<br />

40

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